Resonant averaging for weakly nonlinear stochastic Schrödinger equations

We consider the free linear Schroedinger equation on a torus $\mathbb T^d$, perturbed by a Hamiltonian nonlinearity, driven by a random force and damped by a linear damping: $u_t -iΔu +iνρ|u|^{2q_*}u = - νf(-Δ) u + \sqrtν\,\frac{d}{d t}\sum_{k\in \mathbb Z^d} b_kβ^k(t)e^{ik\cdot x} \ .$ Here $u=u(t,x),\ x\in\mathbb T^d$, $0<ν\ll1$, $q_*\in\mathbb N\cup\{0\}$, $f$ is a positive continuous function, $ρ$ is a positive parameter and $β^k(t)$ are standard independent complex Wiener processes. We are interested in limiting, as $ν\to0$, behaviour of solutions for this equation and of its stationary measure. Writing the equation in the slow time $τ=νt$, we prove that the limiting behaviour of the both is described by the effective equation $u_τ+ f(-Δ) u = -iF(u)+\frac{d}{dτ}\sum b_kβ^k(τ)e^{ik\cdot x} \,$ where the nonlinearity $F(u)$ is made out of the resonant terms of the monomial $|u|^{2q_*}u$. We explain the relevance of this result for the problem of weak turbulence.

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